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“Lighting the Way to Technology through Innovation” The Institute for Lasers, Photonics and Biophotonics University at Buffalo Biophotonics P.N.Prasad www.biophotonics.buffalo.edu
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PHOTOBIOLOGY
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Various Molecular, Cellular and Tissue Components which Interact with Light
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Various Light-Induced Cellular Processes
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The absorption spectra of some important cellular constituents
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The absorption spectra of important cellular constituents The absorption (left) and the fluorescence (right) spectra of important tissue flourophores. The Y-axes represent the absorbance (left) and florescence intensity (right) on a relative scale
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Photoaddition Photofragmentation PHOTOCHEMICAL PROCESSES
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Photooxidation Photoisomerization (Retinal isomerization in the process of vision)
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Retinal isomerization under light exposure
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Various intermediates formed after light absorption by Rhodopsin
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Room temperature time-resolved resonance Raman spectra of rhodopsin and its intermediates. The rhodopsin spectrum is obtained using excitation at 458nm
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Photorearrangement (i)S 0 (photosensitizer) hv S i (photosensitizer) T 1 (photosensitizer) (ii)T 1 (photosensitizer) + T 0 (oxygen) S 0 (photosensitizer) + S 1 (oxygen) (iii)S 1 (oxygen) + A cellular component Photooxidation of the cellular component Photosensitized Oxidation
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Photomedicine: Photodynamic Therapy Photosensitization by Exogenous Molecules
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Photodynamic Therapy Porphyrin Porphyrin + O 2 singlet h O2O2 ( Localizes and accumulates at tumor sites ) Destroys Cancerous Cells
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Mechanism of Photodynamic Photooxidation PDT Drug (P) Light absorption 1 P* 3 P* PDT drug in singlet state PDT drug in triplet state Type I processType II process 3 P* + H 2 0 HO. 3 P* + 3 0 2 1 P + 1 O 2 * Intersystem crossing H2O2H2O2 Oxidation of cellular components cytotoxicity
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Light - Tissue Interactions
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The four possible modes of interaction between light and tissue
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The Various Light Scattering Processes in a Tissue
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I Penetration depths for commonly used laser wavelengths The total intensity attenuation in a tissue can be described as In this equation I(z) is the intensity at a depth z in the tissue; I 0 is the intensity when it enters the tissue; α = absorption coefficient and α s = scattering coefficient. Therefore, α + α s is the total optical loss.
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Light Induced Various Processes in Tissues
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Thermal Laser-Tissue Interaction Photocoagulation: Absorption of visible light generating heat to produce coagulation to seal leaky blood vessels or to repair a tear Thermal keratoplasty: Absorption of IR beam producing heat resulting in shrinkage Photoablation: Photochemical ablation of tissues Photodisruption: Mechanical disruption by creation of plasma PRK, LASIK Posterior capsulotomy Various Laser-Tissue Mechanisms for Ophthalmic Applications
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Various Types of Tissue Engineering using Lasers
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Tattoo removal using laser technology. Four treatments with Q-switched frequency doubled Nd:YAG laser (532nm green) removed the tattoo (Hogan, 2000).
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The Approaches for Tissue Bonding
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Laser tissue ablation using lasers of two different pulse widths. Top: pulse width of 200ps; bottom: pulse width of 80fs (Source: http://www.eecs.umich.edu/CUOS/Medical/Photodisruption.ht ml). FemtoLaser Surgery
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Schematics of various optical interactions with a tissue used for optical biopsy Alfano et al., 1996
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Fluorescence spectra of the normal breast tissue (BN) and the tumor breast tissue (BT) excited at 488 nm In vivo spectroscopy Alfano, R.R. et al., J. Opt. Soc. Am. B. 6:1015-1023 1989
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Raman spectra from normal, benign and malignant breast tumors
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Bioimaging: Principles and Techniques
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Electron Microscopy Nearfield Microscopy, FRET technique Confocal Microscopy, Multiphoton Microscopy, Coherence Tomography etc. Simple microscope, Whole body imaging tools Bio Imaging Tasks : Molecular level to Whole body imaging
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Optical Imaging Confocal Microscopy (CSLM) Multi-photon Microscopy Nearfield Microscopy Optical Coherence Tomography Total Internal Reflection Imaging (TIR) TOOLS Fluorescence Microscopy Raman Imaging ( e.g. CARS) Interference Imaging (e.g. OCT) Techniques Whole body imaging Drug distribution/ Interaction in cells, Organelles or tissue Bio-molecular (e.g. Proteins) activity and organization in cells Identification of Structural changes in cells, organelles, tissues etc. Applications
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Propagation of a laser pulse through a turbid medium
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Confocal and multiphoton imaging. The bottom panel demonstrates the vertical cross-section of the photo-bleached area in a sample.
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Low coherence interferometer. The interference signal as a function of the reference mirror displacement in case of a coherent source (e.g. laser) and a low-coherence source (e.g., SLD) are shown here.
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A table top OCT design using a SLD light source.
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A fiber based OCT design
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1 < c 2 = c 3 > c c : critical angle 11 33 22 Principle of total internal reflection
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Evanescent wave extending beyond the guiding region and decaying exponentially. For waveguiding n 1 > n 2, n 2 = refractive index of surrounding medium. n 1 = refractive index of guiding region.
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Different modes of Near field microscopy
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Schematics of experimental arrangement for obtaining fluorescence spectra from a specific biological site (e.g. organelle) using a CCD coupled spectrograph.
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Fluorescence Polarized Fluorescence Imaging : Fluorescence Resonance Energy Transfer ( FRET ) Fluorescence Recovery After Photobleaching (FRAP) Fluorescence Life time imaging ( FLIM) Molecular diffusion and Mobility measurements in living cells ( e.g. Protein mobility and interactions ) Molecular diffusion and Mobility measurements in living cells ( e.g. Protein mobility and interactions ) Molecular interactions and conformational changes in living cells ( e.g. Protein interactions and conformational changes ) Environmental changes inside cells Complements FRET technique Fluorescence Imaging Techniques
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Nonlinear Optical Techniques Second harmonics Imaging - membrane dynamics - excitation at, signal at 2 CARS Imaging - vibrational imaging - excitation at p and s, signal at 2 p – s with Raman resonance at p – s
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Schematics of a synchronized mode-locked picosecond Ti- Sapphire laser system for backward detection CARS microscopy. Millenia is the diode pumped Nd Laser. Tsunami is the Ti- Sapphire Laser.
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Bioimaging Applications
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Fluorescence labels: Near IR dyes Two-photon emitters Green fluorescent proteins Quantum Dots Rare-earth up-convertors
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Some new Near-IR and IR dyes Commercially available Indocyanine Green, Absorption λ max : 780nm (water), Fluorescence λ max : 805 nm (water) New IR dye *, absorption λ max : 1127 nm (dichloroethane), Emission λ max : 1195nm (dichloroethane) New IR dye *, absorption λ max 1056 nm (dichloroethane), Emission λ max : 1140nm (dichloroethane) *Developed at ILBP
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Lists a chromophore, APSS, and its various derivatives developed at our Institute which can very efficiently be excited at 800 nm and emit in the green ( 520 nm peak)
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Examples of highly efficient two-photon active ionic dyes developed at the Institute for Lasers, Photonics and Biophotonics.
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Excitation and emission spectra of wild type fluorescent protein (FP) as well as the enhanced variants of GFP (eCFP, eGFP, eYFP and eRFP) C = cyan, G = green, y = yellow, R = red
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Three-Photon Excited Amplified Emission pump =1300nm em max =553nm pump He et al., Nature 415, 767 (2002)
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